Abstract

Minimal supersymmetric hybrid inflation based on a minimal Kähler potential predicts a spectral index ns≳0.98. On the other hand, WMAP three year data prefers a central value ns≈0.95. We propose a class of supersymmetric hybrid inflation models based on the same minimal superpotential but with a non-minimal Kähler potential. Including radiative corrections using the one-loop effective potential, we show that the prediction for the spectral index is sensitive to the small non-minimal corrections, and can lead to a significantly red-tilted spectrum, in agreement with WMAP.

Highlights

  • Hybrid inflation models [1, 2] are examples of small field inflation models which predict a very small tensor fraction r ≪ 10−2

  • Amongst the models that are less preferred by the WMAP three year measurement of the spectral index are those based on minimal supersymmetric hybrid inflation

  • In this paper we study supersymmetric hybrid inflation with non-minimal Kahler potential, including radiative corrections using the one-loop effective potential, and show that the prediction of the spectral index is sensitive to such non-minimal effects, which can lead to a significantly red-tilted spectrum

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Summary

Introduction

Hybrid inflation models [1, 2] are examples of small field inflation models which predict a very small tensor fraction r ≪ 10−2. Inflation ends when the field value of the inflaton S falls below some critical value which corresponds to a tachyonic instability for φ and/or φ In this minimal model, the vevs φ and φbreak G to some subgroup H. In this paper we study supersymmetric hybrid inflation with non-minimal Kahler potential, including radiative corrections using the one-loop effective potential, and show that the prediction of the spectral index is sensitive to such non-minimal effects, which can lead to a significantly red-tilted spectrum. The summary is presented in the last section, where we briefly comment on reheating after inflation

Minimal Kahler Potential
Non-Minimal Kahler Potential
Reheating and Baryon Asymmetry

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